Suppose that, and that
for all conjugates
, for some
. Then
is a beta number (and hence
).
The pointsof the orbit correspond to the points
in the lattice
. By the estimates on the conjugates just given, these n points lie in a cube
of volume
, and since the points of the lattice have a constant density in
, there are
points of the lattice in
. By the box principle, for sufficiently large n we must have
for some
and hence the orbit is finite. Once we know the orbit is finite, the conjugates
lie in a finite set, and so certainly
.